Turing patterns on non-fluctuating lattices under mechanical stress modeled by Finsler geometry respond to external forces similarly to those on fluctuating membranes.
From the discrete expression ofH D u ,△uis obtained by the variation ofH D u = ∑i jDu i j(ui −u j)2 in Eq
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Turing patterns on non-fluctuating surfaces under mechanical stresses
Turing patterns on non-fluctuating lattices under mechanical stress modeled by Finsler geometry respond to external forces similarly to those on fluctuating membranes.